the cutoff phenomenon in diffusion processes
DESCRIPTION
A seminar about Cutoff I gave as a student in TorVergataTRANSCRIPT
![Page 1: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/1.jpg)
A short introduction to the cutoff phenomenon indiffusion processes modeled by Markov chains
Carlo Lancia
Mathematical Engineering, University of Rome Tor Vergata
Rome, January 20, 2009
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 2: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/2.jpg)
Outline
1 IntroductionMarkov Chains, Stationarity and Total Variation DistanceTop-at-Random ShuffleDefinition of Cutoff
2 Ehrenfest’s Urn ModelModel OverviewNumerical DataA Model for the Second Law of Thermodynamics
3 Random WalksCircular Random WalkLinear Random WalkBiased Linear Random Walk
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 3: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/3.jpg)
Introduction Markov Chains, Stationarity and TV Distance
Some Definitions
Finite Markov Chain: a sequence of random variablesX0, X1, . . . , Xt, . . . taking values in Ω = 1, 2, . . . , nTransition Matrix: a n× n matrix Pij such that
P(Xt+1 = j|Xt = i) = Pij
Total Variation Distance: if λ, µ are two probabilitydistribution over Ω,
dTV (λ, µ) :=12
n∑i=1
|µ(i)− λ(i)| = supA⊂Ω
∣∣∣∣∣∑i∈A
[µ(i)− λ(i)]
∣∣∣∣∣Stationary Distribution π: probability distribution of thestationary state, π = π P
Mixing Time τ(ε): first time t such that dTV (P ti0 , π) ≤ ε
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 4: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/4.jpg)
Introduction Markov Chains, Stationarity and TV Distance
Total Variation Distance
Two distributions are close in total variation if and only ifthey are uniformly close on all subsets
ExampleLet’s suppose we succeeded in well-shuffling a deck of 52cards. Well-shuffling a deck means to sample uniformly atrandom one of 52! possible cards permutations.What happens if we see the bottom card of the deck, say theace of spades, A♠?
We loose uniformityNow the deck is arranged according to the uniform distribution overthe 51! possible permutations of 52 cards, last of them being A♠
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 5: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/5.jpg)
Introduction Markov Chains, Stationarity and TV Distance
Total Variation Distance
Two distributions are close in total variation if and only ifthey are uniformly close on all subsets
ExampleLet’s suppose we succeeded in well-shuffling a deck of 52cards. Well-shuffling a deck means to sample uniformly atrandom one of 52! possible cards permutations.What happens if we see the bottom card of the deck, say theace of spades, A♠?
We loose uniformityNow the deck is arranged according to the uniform distribution overthe 51! possible permutations of 52 cards, last of them being A♠
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 6: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/6.jpg)
Introduction Markov Chains, Stationarity and TV Distance
Total Variation Distance
Two distributions are close in total variation if and only ifthey are uniformly close on all subsets
ExampleLet’s suppose we succeeded in well-shuffling a deck of 52cards. Well-shuffling a deck means to sample uniformly atrandom one of 52! possible cards permutations.What happens if we see the bottom card of the deck, say theace of spades, A♠?
We loose uniformityNow the deck is arranged according to the uniform distribution overthe 51! possible permutations of 52 cards, last of them being A♠
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 7: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/7.jpg)
Introduction Markov Chains, Stationarity and TV Distance
Total Variation Distance
Pay attention when dealing with total variation distanceThe total variation distance of the new deck distribution from theuniform one is (
151!− 1
52!
)51! = 1− 1
52≈ 0.98
Total variation distance can be very unforgiving of smalldeviations from uniformity.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 8: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/8.jpg)
Introduction Top-at-Random Shuffle
Top-at-Random Shuffle
Top in at Random is the simplest model of card shuffling:A random position of the deck is chosenTop card is inserted into the deck at that positionProcess is iterated until convergence
Single iteration of the shuffling processUntil convergence meansunitl cards are arrangedaccording to the uniformdistribution over the n!deck permutations
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 9: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/9.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
We follow the bottom card of a deck of size nThis card stays at the bottom until the first time T1 a card isinserted below it;Consider the instant T2 when a second card is inserted belowthe original bottom card. The two cards under the originalbottom card are equally likely to be in relative order low-highor high-low;At time Tn−1 the original bottom card comes up to the top.By an inductive argument, all (n− 1)! arrangements of thelower cards are equally likely;When the original bottom card is inserted at random, at timeTn = Tn−1 + 1, then all n! possible arrangements of the deckare equally likely.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 10: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/10.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
We follow the bottom card of a deck of size nThis card stays at the bottom until the first time T1 a card isinserted below it;Consider the instant T2 when a second card is inserted belowthe original bottom card. The two cards under the originalbottom card are equally likely to be in relative order low-highor high-low;At time Tn−1 the original bottom card comes up to the top.By an inductive argument, all (n− 1)! arrangements of thelower cards are equally likely;When the original bottom card is inserted at random, at timeTn = Tn−1 + 1, then all n! possible arrangements of the deckare equally likely.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 11: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/11.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
We follow the bottom card of a deck of size nThis card stays at the bottom until the first time T1 a card isinserted below it;Consider the instant T2 when a second card is inserted belowthe original bottom card. The two cards under the originalbottom card are equally likely to be in relative order low-highor high-low;At time Tn−1 the original bottom card comes up to the top.By an inductive argument, all (n− 1)! arrangements of thelower cards are equally likely;When the original bottom card is inserted at random, at timeTn = Tn−1 + 1, then all n! possible arrangements of the deckare equally likely.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 12: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/12.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
We follow the bottom card of a deck of size nThis card stays at the bottom until the first time T1 a card isinserted below it;Consider the instant T2 when a second card is inserted belowthe original bottom card. The two cards under the originalbottom card are equally likely to be in relative order low-highor high-low;At time Tn−1 the original bottom card comes up to the top.By an inductive argument, all (n− 1)! arrangements of thelower cards are equally likely;When the original bottom card is inserted at random, at timeTn = Tn−1 + 1, then all n! possible arrangements of the deckare equally likely.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 13: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/13.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
We follow the bottom card of a deck of size nThis card stays at the bottom until the first time T1 a card isinserted below it;Consider the instant T2 when a second card is inserted belowthe original bottom card. The two cards under the originalbottom card are equally likely to be in relative order low-highor high-low;At time Tn−1 the original bottom card comes up to the top.By an inductive argument, all (n− 1)! arrangements of thelower cards are equally likely;When the original bottom card is inserted at random, at timeTn = Tn−1 + 1, then all n! possible arrangements of the deckare equally likely.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 14: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/14.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
Expectation of Tk : E[Tk] =n∑j=1
j P(Tk = j) =n
k
Mixing Time Estimate: E[τ ] = 1 +n−1∑k=1
E[Tk] = n log n
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 15: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/15.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
Expectation of Tk : E[Tk] =n∑j=1
j P(Tk = j) =n
k
Mixing Time Estimate: E[τ ] = 1 +n−1∑k=1
E[Tk] = n log n
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 16: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/16.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
Expectation of Tk : E[Tk] =n∑j=1
j P(Tk = j) =n
k
Mixing Time Estimate: E[τ ] = 1 +n−1∑k=1
E[Tk] = n log n
Convergence of Top at Random modelUntil time Tn−1 we may have knowledge of the exact position ofthe original bottom card, so dTV (P t, π) ≈ 1 if t < Tn−1. At timeTn cards are arranged according to the uniform distribution, sodTV (P t, π) ≈ 0 if t > Tn.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 17: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/17.jpg)
Introduction Top-at-Random Shuffle
Top-in-at-Random Analysis
Expectation of Tk : E[Tk] =n∑j=1
j P(Tk = j) =n
k
Mixing Time Estimate: E[τ ] = 1 +n−1∑k=1
E[Tk] = n log n
A sharp evaluation of τThe chain abruptly converges to stationarity at time Tn son log n is actually discovered to be not only a mean valuebut a also very sharp evaluation of τ .
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 18: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/18.jpg)
Introduction Definition of Cutoff
The Cutoff Phenomenon
We consider a family of chains X(n)t ∈ Ωn = 1, 2, . . . , n
The n-th chain has transition kernel P (n), limit measure πn andmixing time τ (n)(ε). P tn is the state distribution after t steps.
Let an, bn be two sequences such thatbnan→ 0.
Definition
The family Ωn, X(n)t , πn exhibits cutoff at time an with a cutoff
window of size bn iff
limθ→∞
lim supn→∞
‖P dan+θbnen − πn‖TV = 0
limθ→∞
lim infn→∞
‖P ban−θbncn − πn‖TV = 1
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 19: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/19.jpg)
Introduction Definition of Cutoff
The Case of Birth-and-Death Chains
Xt is a birth-and-death chain if Pij = 0 unless |i− j| ≤ 1Xt is a δ-lazy birth-and-death chain provided Pii = δ > 0
Definition
A family of birth-and-death chains Ωn, X(n)t , πn exhibits cutoff iff
limn→∞
τ (n)(ε)τ (n)(1− ε)
= 1 ∀ 0 < ε < 1
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 20: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/20.jpg)
Introduction Definition of Cutoff
Cutoff for Birth-and-Death Chains
whether a family of δ-lazy birth-and-death chains exhibits cutoff itdepends on the product τ (n) · t(n)
rel
t(n)rel is the relaxation time and is equal to (1− λn)−1
λn is the largest absolute-value of all nontrivial eigenvalues ofthe transition kernel P (n) (nontrivial means different from 1)
TheoremA family of δ-lazy birth-and-death chains exhibits cutoff ifft(n)rel = o(τ (n)(1
4)) and
τ (n)(1− ε)− τ (n)(ε) ≤
√t(n)rel · τ (n)
(14
)
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 21: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/21.jpg)
Ehrenfest’s Urn Model Model Overview
Ehrenfest’s Urn Model
The Ehrenfest’s Urn is a very simple model for particles diffusion.We have n balls in 2 urns
A ball is randomly chosen and moved to the other urnProcess is iterated towards stationarity
Single chain step Say Xt is the number ofballs in urn 1, then Xt isan ergodic Markov chainwhich limit measure is
π(j) = 2−n(nj
)
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 22: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/22.jpg)
Ehrenfest’s Urn Model Numerical Data
Cutoff for the Ehrenfest’s Urn Model
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 23: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/23.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 24: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/24.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 25: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/25.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 26: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/26.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 27: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/27.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 28: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/28.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 29: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/29.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 30: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/30.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 31: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/31.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 32: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/32.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 33: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/33.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 34: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/34.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 35: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/35.jpg)
Ehrenfest’s Urn Model Numerical Data
Evolution of the Distribution Curve
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 36: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/36.jpg)
Ehrenfest’s Urn Model A Model for the Second Law of Thermodynamics
Explaining the Second Law of Thermodynamics
How can entropy increase be compatible with a systemreturning to its starting state?
Suppose entropy is measured by
I(t) =n∑j=0
P t0 logP t0
where P t0 is the distribution of the number of balls in urn 1 after tsteps, urn 1 being initially empty.
I(t) is increasing in t because the system tends to stationarity;It is equally certain that the number of balls in urn 1 willreturn to zero infinitely often as time goes on.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 37: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/37.jpg)
Ehrenfest’s Urn Model A Model for the Second Law of Thermodynamics
Explaining the Second Law of Thermodynamics
How can entropy increase be compatible with a systemreturning to its starting state?
Suppose entropy is measured by
I(t) =n∑j=0
P t0 logP t0
Return to initial position won’t be observedIt takes about n log n steps for the chain to reach maximum entropybut about 2n steps to have a reasonable chance of returning to 0.If n is large (Avogadro’s number) we will not observe suchreturns
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 38: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/38.jpg)
Random Walks Circular Random Walk
Lazy Uniform Random Walk mod n
This process is clearly a 13 -lazy birth-and-death chain, Ω = Z mod n
πn ≡ 1n
τ (n) = O(n2)
t(n)rel = O(n2)
=⇒ NO CUTOFF
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 39: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/39.jpg)
Random Walks Circular Random Walk
Lazy Uniform Random Walk mod n
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 40: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/40.jpg)
Random Walks Linear Random Walk
Lazy Uniform Random Walk
Also this process is a 13 -lazy birth-and-death chain, Ω = 1, . . . , n
πn ≡ 1n
τ (n) = O(n2)
t(n)rel = O(n2)
=⇒ NO CUTOFF
Regularity of dTVSince π is uniform dTV (P t, π) smoothlydecreases from 1 to 0 wherever thechain starts at t = 0
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 41: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/41.jpg)
Random Walks Linear Random Walk
Lazy Uniform Random Walk
Also this process is a 13 -lazy birth-and-death chain, Ω = 1, . . . , n
πn ≡ 1n
τ (n) = O(n2)
t(n)rel = O(n2)
=⇒ NO CUTOFF
Regularity of dTVSince π is uniform dTV (P t, π) smoothlydecreases from 1 to 0 wherever thechain starts at t = 0
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 42: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/42.jpg)
Random Walks Linear Random Walk
Lazy Uniform Random Walk
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 43: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/43.jpg)
Random Walks Biased Linear Random Walk
Biased Lazy Uniform Random Walk
What happens if we break the transition probabilities symmetry?
DriftWe introduce a drift q > 0, so the chain has abigger chance to move right
Breaking symmetry leads to cutoffBreaking symmetry concentrates π on the right wall.If the chain starts from the left we detect cutoff.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 44: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/44.jpg)
Random Walks Biased Linear Random Walk
Biased Lazy Uniform Random Walk
What happens if we break the transition probabilities symmetry?
DriftWe introduce a drift q > 0, so the chain has abigger chance to move right
Breaking symmetry leads to cutoffBreaking symmetry concentrates π on the right wall.If the chain starts from the left we detect cutoff.
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 45: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/45.jpg)
Random Walks Biased Linear Random Walk
Biased Lazy Uniform Random Walk
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 46: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/46.jpg)
Random Walks Biased Linear Random Walk
Biased Lazy Uniform Random Walk
Carlo Lancia Short Introduction to the Cutoff Phenomenon
![Page 47: The cutoff phenomenon in diffusion processes](https://reader030.vdocument.in/reader030/viewer/2022020207/55990eeb1a28ab0b2c8b4613/html5/thumbnails/47.jpg)
Random Walks Biased Linear Random Walk
Biased Lazy Uniform Random Walk
Carlo Lancia Short Introduction to the Cutoff Phenomenon